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Raman spectroscopy characterisation of oriented bundles of single-crystal rutile-phase TiO2 nanorods prepared by hydrothermal bath deposition on transparent conducting substrates
Rutile-phase TiO 2 rods prepared by hydrothermal bath deposition on F:SnO 2 are in fact bundles of single-crystal TiO 2 prismatic nanorods of ~ 4 nm diameter each. These bundles of rutile-phase TiO 2 nanorods have tetragonal morphology and are strain-free (or the strain in all the samples is the sam...
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Published in: | Applied physics. A, Materials science & processing Materials science & processing, 2019-06, Vol.125 (6), p.1-10, Article 389 |
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Main Authors: | , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Rutile-phase TiO
2
rods prepared by hydrothermal bath deposition on F:SnO
2
are in fact bundles of single-crystal TiO
2
prismatic nanorods of ~ 4 nm diameter each. These bundles of rutile-phase TiO
2
nanorods have tetragonal morphology and are strain-free (or the strain in all the samples is the same). Bundles of TiO
2
that are oriented tetragonally with respect to the substrate’s surface, can be prepared for optimized growth times. It is observed that bundles of TiO
2
nanorods act as single entities from the point of view of the Raman spectra (and thus lattice vibrations). Single prismatic nanorods of ~ 4 nm width, as observed via TEM, appear to act as “larger” crystals to the lattice phonons once stacked together to form large oriented bundles of TiO
2
. Hence, the phonon confinement effect cannot be observed because translational symmetry is preserved at the grain boundaries of the nanorods that make each TiO
2
bundle. Moreover, an increase in the density of bundles growing preferentially in the [002] direction, perpendicular to the substrate surface, results in an unusual increase of room and low (77 K) temperature Raman band
E
g
/
A
1g
intensity ratios. |
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ISSN: | 0947-8396 1432-0630 |
DOI: | 10.1007/s00339-019-2688-4 |